
independent of the \((ql)\)  index by following the formula in Ref. [1]}, (see, also Refs. [2]}, [3]}, [4]}).
Hence, the LHC bounds of \(C_X^{ql} (m_b)\)  are easily obtained by rescaling our results in Fig. REF .
The \(S_2\) -\(T\)  mixing propagates \(C_{S_2} (\rm {\Lambda _{LHC}})\)  and \(C_T (\rm {\Lambda _{LHC}})\)  to \(C_{S_2} (m_b)\) .
